<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">ACES</journal-id><journal-title-group><journal-title>Advances in Chemical Engineering and Science</journal-title></journal-title-group><issn pub-type="epub">2160-0392</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/aces.2013.31001</article-id><article-id pub-id-type="publisher-id">ACES-26465</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Chemistry&amp;Materials Science</subject></subj-group></article-categories><title-group><article-title>
 
 
  Effect of Two Liquid Phases on the Separation Efficiency of Distillation Columns
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ardênia</surname><given-names>Marinho Cordeiro</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Stephanie</surname><given-names>Rolim Dantas</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Luís</surname><given-names>Gonzaga Sales Vasconcelos</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Romildo</surname><given-names>Pereira Brito</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Chemical Engineering, Federal University of Campina Grande, Campina Grande, Brazil</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>romildo.brito@deq.ufcg.edu.br(RPB)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>01</month><year>2013</year></pub-date><volume>03</volume><issue>01</issue><fpage>1</fpage><lpage>8</lpage><history><date date-type="received"><day>September</day>	<month>5,</month>	<year>2012</year></date><date date-type="rev-recd"><day>October</day>	<month>7,</month>	<year>2012</year>	</date><date date-type="accepted"><day>October</day>	<month>16,</month>	<year>2012</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   Distillation is one of the oldest and most important separation processes used in the chemical and petrochemical industries. On the other hand, it is a process the thermodynamic efficiency of which is very low, and therefore reducing the consumption of energy is one of the targets of research studies on distillation. This article arose from seeking to reduce energy consumption in a distillation train of 1,2-dichloroethane (ethylene dichloride-EDC) of a commercial plant producing vinyl monochloride (VMC), which involves an azeotropic distillation column. The reduction in the reboiler heat duty caused significant changes in concentration and temperature profiles throughout the column due to the formation of two liquid phases. The results show that, although very small in percentage terms (less than 2.5%), the appearance of the 2<sup>nd</sup> liquid phase causes significant changes in the operation of the column and the separation achieved.
     
 
</p></abstract><kwd-group><kwd>Distillation; Azeotropic; Two Liquid Phases; Separation Factor</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Distillation is one of the oldest and most important separation processes used in chemical processes. On the other hand, its thermodynamic efficiency is extremely low, which accounts for the high percentage of global energy consumed in a plant. In general, distillation column reboilers consume over 50% of the energy involved in the process of heat exchange in a plant (Soave and Feliu, 2002 [<xref ref-type="bibr" rid="scirp.26465-ref1">1</xref>]).</p><p>The term azeotropic distillation is applied to the class of techniques based on fractional distillation in which azeotropic behavior is exploited to achieve separation. Traditionally, the specie that causes the azeotropic behavior is added as a mass separating agent: the entrainer. In some situations it may be present in the feed mixture (self-entraining) of the azeotropic column (Perry et al., 1999 [<xref ref-type="bibr" rid="scirp.26465-ref2">2</xref>]).</p><p>Although a large number of studies involve azeotropic distillation, most involve columns in which a third component is added in order to further the separation. Such studies are about choosing the third component, the influence of a thermodynamic model, evaluating the existence of multiple steady states and the study of process control (Laroche et al., 1992 [<xref ref-type="bibr" rid="scirp.26465-ref3">3</xref>]; Bekiaris et al., 2000 [<xref ref-type="bibr" rid="scirp.26465-ref4">4</xref>]; Magnussen et al., 1979 [<xref ref-type="bibr" rid="scirp.26465-ref5">5</xref>]; Rovaglio and Doherty, 1990 [<xref ref-type="bibr" rid="scirp.26465-ref6">6</xref>]; Wang et al., 1997 [<xref ref-type="bibr" rid="scirp.26465-ref7">7</xref>]; Luyben, 2008 [<xref ref-type="bibr" rid="scirp.26465-ref8">8</xref>]; Wu and Chien, 2009 [<xref ref-type="bibr" rid="scirp.26465-ref9">9</xref>]). Another striking feature of the articles cited is that they consider the formation of two liquid phases only in the reflux vessel.</p><p>Lao and Taylor (1994) [<xref ref-type="bibr" rid="scirp.26465-ref10">10</xref>] reviewed the literature on the separation efficiency of distillation columns involving three-phase systems, and cite several sources which give rise to their finding that the conclusions drawn on these systems are contradictory. Some studies claim that overall efficiency was not influenced by the number of liquid phases present. Other studies indicate that the introduction of a second liquid phase may have a strong (positive or negative) influence on the mass transfer.</p><p>Widagdo and Seider (1996) [<xref ref-type="bibr" rid="scirp.26465-ref11">11</xref>] published one of the most complete (and even to this day, one of the most cited) articles on the azeotropic distillation process. They showed that knowledge contained in the literature is scant both as to a real understanding of the process and the difficulties regarding control of azeotropic columns. They also emphasized the issue of the formation of two liquid phases within the column, but there is no consensus on the efficiency of separation when columns operating with one and with two liquid phases are compared.</p><p>In 1997 Wang et al. [<xref ref-type="bibr" rid="scirp.26465-ref7">7</xref>] observed experimentally the formation of two liquid phases inside a column, depending on the reflux and the reboiler heat duty, as well as the presence of multiple steady states; the study evaluated the dehydration of isopropanol, using cyclohexane as the entrainer.</p><p>According to Higler et al. (2004) [<xref ref-type="bibr" rid="scirp.26465-ref12">12</xref>], azeotropic distillation is characterized by its operational complexity, due to the possible formation of two liquid phases inside the column. The authors used an equilibrium and a non-equilibrium stage model and claimed the formation of two liquid phases in the distillation column influences the mass transfer process, thus affecting efficiency.</p><p>The equilibrium stage model, widely used in modeling and simulating distillation processes, does not represent the reality that few stages actually operate in equilibrium. This problem can be solved by introducing Murphree efficiencies. However, some authors (Cairns and Furzer, 1990 [<xref ref-type="bibr" rid="scirp.26465-ref13">13</xref>]) warned against incorporating Murphree efficiencies into equilibrium stage models of three-phase systems. In fact, the projections may be more accurate if a non-equilibrium stage model is considered. However, calculations are complex, thus requiring more computational time, which is not desirable for control applications. But, the biggest obstacle is that the parameters required to perform the calculations are rarely available.</p><p>Junqueira et al. (2009) [<xref ref-type="bibr" rid="scirp.26465-ref14">14</xref>] analyzed the formation of two liquid phases in the azeotropic column in the production of anhydrous ethanol, and, in order to decrease this phenomenon, many process configurations have been studied as well as variations in operating conditions. It was concluded that the formation of the second liquid phase may affect the performance of the column and consequently reduce its efficiency.</p><p>Silva et al. (2003) [<xref ref-type="bibr" rid="scirp.26465-ref15">15</xref>] evaluated the dynamics of an azeotropic distillation column similar to the one considered in this article; however, the entrainer was already present in the feed, which was held in the intermediate region of the column, and the formation of two liquid phase occurred only in the reflux vessel.</p><p>Guedes et al. (2007) [<xref ref-type="bibr" rid="scirp.26465-ref16">16</xref>] followed the same procedure as the one studied in this paper and, in the steady state, evaluated the process sensitivity relative to the feed temperature; and, dynamically evaluated the influence in feed temperature, including the operation condition with two liquid phases in some plates.</p><p>The distillation column considered in this article shows characteristics of an azeotropic distillation, since two liquid phases form in the reflux vessel and, depending on the operation condition, in some stages throughout the column. However, another feature makes the system unconventional: the feed takes place in the reflux vessel. In the research literature few studies have considered systems with these characteristics.</p></sec><sec id="s2"><title>2. Problem Statement</title><p>The distillation column considered in this study is part of the purification train of 1,2-dichloroethane (ethylene dichloride-EDC) of a commercial plant which produces vinlyl chloride monomer (VCM).</p><p>The process of obtaining EDC occurs through the direct chlorination of ethylene (C<sub>2</sub>H<sub>4</sub>), as shown in the reaction: C<sub>2</sub>H<sub>4</sub> + Cl<sub>2</sub> &#174; C<sub>2</sub>H<sub>4</sub>Cl<sub>2</sub>. The EDC product (high purity) leaves the reactor and moves on to the purification system, where it undergoes aqueous washing. <xref ref-type="fig" rid="fig1">Figure 1</xref> shows the flow diagram of the EDC dehydration process, where it can be observed that aqueous washing is conducted in the separating vessel (or reflux vessel). After the top condenser and in the reflux vessel, there are two liquid phases: an organic one, saturated in H<sub>2</sub>O, and an aqueous one, saturated in organic matter. The organic phase returns to the reflux of the column, while the stream of the aqueous phase is discarded.</p><p>Although less volatile than the EDC, the H<sub>2</sub>O leaves from the top of the column due to the reversal in the value of the constant K (<xref ref-type="fig" rid="fig2">Figure 2</xref>), which is due to the fact that H<sub>2</sub>O forms a minimal azeotrope, not only with the EDC, but with almost all organic compounds present in the process.</p><p>Note that in the stream coming from the reactor (FROMR1) there is no H<sub>2</sub>O, so that during washing, the stream that carries out the reflux of the column (TODRY 2) becomes saturated in H<sub>2</sub>O.</p><p>A close analysis of <xref ref-type="fig" rid="fig1">Figure 1</xref> leads to the conclusion that the system as a whole can be seen as a conventional column (with reboiler, condenser and reflux vessel), with the feed (FROMR1 and WATER) in the reflux vessel. In industry, although the analysis of the degree of freedom indicates two variables will be manipulated, only the reboiler heat duty is used, since the reflux flow rate is used to control the level (organic phase) of the vessel and the distillate flow rate (WASTE) cannot return to the process.</p><p>The study by Guedes et al. (2007) [<xref ref-type="bibr" rid="scirp.26465-ref16">16</xref>] aimed at reducing the consumption of energy in the azeotropic column. The question to be answered was: if the reboiler heat duty is the only manipulated variable used, to what extent can it be reduced without compromising the quality of the bottom product (the H<sub>2</sub>O mass fraction)?</p><p>Accordingly, by performing tests in the plant, the reboiler heat duty was gradually reduced, which resulted in plate temperatures (top, middle and bottom) that were much smaller than those observed historically, being indicated. In spite of the amount of moisture in the bottom stream being below the specification (10 ppm), the tests were discontinued after 7 hours of operation, and a new operating condition (lower heat duty) was established.</p><p>According to Guedes et al. (2007) [<xref ref-type="bibr" rid="scirp.26465-ref16">16</xref>], a more significant change in the temperature profile occurs because of the formation of a 2<sup>nd</sup> liquid (aqueous) phase in the plates of the column. And, the good agreement between</p><p>azeotropic data (Azeotropic Data, 1973 [<xref ref-type="bibr" rid="scirp.26465-ref17">17</xref>]) and solubility (Dechema, 1990) found in the literature for EDC-H<sub>2</sub>O and those predicted by the simulations, are the mainstays of this conclusion. However, the simulations were carried out without formally defining an objective function and constraints (optimization). Furthermore, no evaluation of the effect of the possible presence of a 2<sup>nd</sup> liquid phase in separation was performed. Thus, this study aimed to: formalize optimizing the consumption of energy, and evaluate the efficiency of separation taking two operating conditions into account: without the formation of two liquid phases (Case I) and with the formation of two liquid phases (Case II).</p></sec><sec id="s3"><title>3. Modeling and Simulation</title><p>The simulation was performed using Aspen Plus<sup>TM</sup> commercial simulator. In order to represent the real system, the system was modeled using reboiled absorption, followed by a condenser (Heater) and a decanter (Decanter). To model the column in question, the RadFrac™ routine was used.</p><p>The RadFrac<sup>TM</sup> routine detects the possible formation of a second liquid phase (the main component was H<sub>2</sub>O) at any stage; assumes there is an equilibrium stage model; and uses specified values for stage efficiencies. These efficiencies can be manipulated to adapt to the plant data. In this study, a Murphree efficiency equal to 64% for all plates and 100% for the reboiler was used. In the industrial plant, the column has 25 stages (numbered from top to bottom) and a reboiler type thermosyphon. In the Aspen Plus<sup>TM</sup> simulator, the pressure in each plate of the column, as well as in the other equipment, is kept constant.</p><p>To represent the equilibrium between liquid-liquidvapor phases (ELLV), a γ-φ procedure was used. Even with the column operating under low pressure, the vapor phase was represented by the Redlich-Kwong Equation of State (EOS). The activity coefficient γ was determined from the NRTL model (Perry et al., 1999 [<xref ref-type="bibr" rid="scirp.26465-ref2">2</xref>]), which represents the ELLV system effectively. Tables 1 and 2, respectively, show the comparison between the azeotropic (Azeotropic Data, 1973) and solubility data (Dechema, 1990 [<xref ref-type="bibr" rid="scirp.26465-ref18">18</xref>]) found in the literature for the EDC-H<sub>2</sub>O system (main components) and those predicted by the simulations.</p><p>In order to determine the optimal energy consumption, the objective function (J) to be minimized was defined as the reboiler heat duty (Qr).</p><p>The restriction in the case of optimization without the presence of two liquid phases (Case I) is the mass fraction of H<sub>2</sub>O in the liquid phase (global): if it was not desired to form two liquid phases over the column, the restriction imposed was 2500 Parts Per Million (ppm) (approximately the saturation value of EDC with H<sub>2</sub>O at 45˚C) for the first stage (numbered from top to bottom) of the column. The choice of this plate was due to its being found that the formation of two liquid phases starts in this plate.</p><p>For the operation with two liquid phases (Case II), the restriction imposed was 10 ppm in the bottom stream of the column (the maximum permitted in the plant). Mathematically, the problem was formulated as follows:</p><disp-formula id="scirp.26465-formula6309"><label>(1)</label><graphic position="anchor" xlink:href="1-3700230\0a424035-b2f4-46ab-9dc9-e4dafa4761b5.jpg"  xlink:type="simple"/></disp-formula><p>Subject to</p><disp-formula id="scirp.26465-formula6310"><label>(2)</label><graphic position="anchor" xlink:href="1-3700230\b3d6c2d8-5144-4c31-820a-97a231bd3327.jpg"  xlink:type="simple"/></disp-formula><p>Or</p><disp-formula id="scirp.26465-formula6311"><label>(3)</label><graphic position="anchor" xlink:href="1-3700230\e5e8a794-796d-4feb-9ffe-2dff1997f1e2.jpg"  xlink:type="simple"/></disp-formula><p>The optimization procedure considered the distillate flowrate (stream OCSUM1) as the manipulated variable</p><p><xref ref-type="table" rid="table1">Table 1</xref>. Comparison of azeotropic data for EDC(1)-H<sub>2</sub>O(2) system.</p><p><img src="1-3700230\72c20937-cd4c-4974-932c-c04f83a9c8ba.jpg" /></p><p><xref ref-type="table" rid="table2">Table 2</xref>. Solubility (% weight) of EDC(1)-H<sub>2</sub>O(2) system.</p><p><img src="1-3700230\ca726629-bee4-4ef3-8070-a69e6a45b5d6.jpg" /></p><p>(OCSUM1). The objective function was inserted via the Analysis/Optimization Model of the Aspen Plus<sup>TM</sup> tool, which uses the Sequential Quadratic Programming (SQP) search method for the optimum. The restrictions were inserted using the Analysis/Constraint Model.</p><p>The procedure can be implemented over the following steps:</p><p>1) Fix the number of stages of the column;</p><p>2) Specify the value of the distillate flowrate, which will be used as an initial estimate;</p><p>3) Insert, via the Analysis/Optimization Model, the objective function and the range over which the variable may be manipulated;</p><p>4) Insert, via the Analysis Constraint Model, the restriction and its tolerance.</p></sec><sec id="s4"><title>4. Steady-State Results</title><p>A comparison of data from the plant (the historical operating conditions) and those provided by the simulation is shown in <xref ref-type="table" rid="table3">Table 3</xref>. The good agreement between real and simulated data, in fact, proves the effectiveness of the modeling and the simulation.</p><p><xref ref-type="table" rid="table4">Table 4</xref> shows the conditions of the stream from the reactor (FROMR1) and <xref ref-type="table" rid="table5">Table 5</xref> presents results for two operating conditions: 1) historical and 2) optimized.</p><p>As per <xref ref-type="table" rid="table5">Table 5</xref>, with the formation of two liquid phases (Case II), the reduction in energy consumption compared with the situation with a single liquid phase (Case I) is 19.4%; a result caused by a decrease in the distillate flow rate.</p><p>The final value of the reboiler heat duty was derived and determined after the constraints were optimized. In both cases, the production of “dry” EDC (EDCDRY2) was very similar.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref>, note the large difference between the temperature profiles for the two optimal situations. For Case I, a significant variation occurs between the 1<sup>st</sup> and the 5<sup>th </sup>plate, and then the rate of increase is almost linear from there to the 26<sup>th</sup> plate (bottom). On the other hand, in case II, the variation in the rate of increase between the 1<sup>st </sup>and 16<sup>th</sup> plate is almost linear, and then there are steep increases in this rate until the 24<sup>th</sup> plate at which point the temperatures in the two cases coincide.</p><p><xref ref-type="table" rid="table3">Table 3</xref>. Comparison between the real and simulation data (Guedes et al., 2007).</p><p><img src="1-3700230\d17bdf03-db39-4642-8b5f-7bd4fe6a92b3.jpg" /></p><p><xref ref-type="table" rid="table4">Table 4</xref>. Characteristics of the feed (FROMR1).</p><p><img src="1-3700230\90369415-7809-4b54-b5d5-561a1fde4363.jpg" /></p><p><xref ref-type="table" rid="table5">Table 5</xref>. Results for two operational conditions.</p><p>In both cases, the linear behavior of the temperature takes place basically by varying the pressure, since the change in the composition of the species along the column is very small, as shown in <xref ref-type="fig" rid="fig4">Figure 4</xref>. Simulations that include a negligible pressure drop along the column show the temperature profiles then remain on plateaus, rather than go straight upward, thus confirming this observation on the result of there being negligible drops in the pressure. The profiles obtained experimentally by Wang et al. (1997) [<xref ref-type="bibr" rid="scirp.26465-ref7">7</xref>] show qualitative forms similar to <xref ref-type="fig" rid="fig3">Figure 3</xref>. However, unlike the findings of this study, the</p><p>percentage of H<sub>2</sub>O present in the feed was high.</p><p><xref ref-type="fig" rid="fig4">Figure 4</xref> shows the mass fraction of EDC and H<sub>2</sub>O (main components) in each stage, from which it may be seen that, in each case, the mass transfer is at its most significant in different regions of the column: for Case I in the upper region; for Case II, in the lower one. For Case II, the greatest change in composition occurs in the region where the 2<sup>nd</sup> liquid phase is not present (from the 16<sup>th</sup> stage on). In fact, in both cases, dehydration mainly occurs in a small region of the column.</p><p>Given the low transfer of mass in most of the column, <xref ref-type="fig" rid="fig4">Figure 4</xref> suggests that the number of stages of the column could be smaller. In fact, if the reboiler heat duty is maintained constant, simulations for a column with 19 stages show the presence of a single liquid phase and the fraction of H<sub>2</sub>O at the bottom is within specification. However, for columns with 18 stages, two phases are present and the liquid fraction of H<sub>2</sub>O at the bottom (1000 ppm) is above the one laid down in the specification.</p><p>The reason for the formation of two liquid phases can be seen in <xref ref-type="fig" rid="fig4">Figure 4</xref>. For Case II, in the region of two liquid phases, the maximum mass fraction of H<sub>2</sub>O is about 0.7% by weight, so it is above the saturation value of the organic phase with H<sub>2</sub>O. For Case I, the maximum mass fraction of H<sub>2</sub>O is around 0.25% by weight (approximately the saturation value of EDC with H<sub>2</sub>O). The behavior of Case II is due to the fact that the decrease in the reboiler heat duty does not prompt the removal of H<sub>2</sub>O (in the form of azeotrope) in the early stages of the column.</p><p><xref ref-type="fig" rid="fig5">Figure 5</xref> shows the Separation Factor (SF) defined by Equation (4) Perry et al., 1999 [<xref ref-type="bibr" rid="scirp.26465-ref2">2</xref>]) along the column, in which what can be noted is that the separation efficiency is increased when there is a single liquid phase. Even if the second liquid phase is present, the Separation Factor is greater in stages where this phase disappears. From this Figure, note also that, for Case II (a two liquid phase up to plate 16), dehydration occurs in the last few plates. Overall, the magnitude of the Separation Factor measured for Case I (1.15E9) was completely different from that calculated for Case II (235).</p></sec></body><back><ref-list><title>References</title><ref id="scirp.26465-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G. Soave and J. A. Feliu, “Saving Energy in Distillation by Feed Splitting,” Applied Thermal Engineering, Vol. 22, No. 8, 2002, pp. 889-896.</mixed-citation></ref><ref id="scirp.26465-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">R. H. Perry, D. W. Green and J. O. Maloney, “Perry’s Chemical Engineer’s Handbook,” 7th Edition, McGraw-Hill, New York, 1999.</mixed-citation></ref><ref id="scirp.26465-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">L. Laroche, N. Bekiaris, H. W. Andersen and M. Morari, “The Curious Behaviour of Homogeneous Azeotropic Distillation—Implications for Entrainer Selection,” AIChE Journal, Vol. 38, No. 9, 1992, pp. 1309-1328.</mixed-citation></ref><ref id="scirp.26465-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">N. Bekiaris, E. G. Guttinger and M. Morari, “Multiple Steady States in Distillation: Effect of VL(L)E Inaccuracies,” AIChE Journal, Vol. 46, No. 5, 2000, pp. 955-979.</mixed-citation></ref><ref id="scirp.26465-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">T. M. Magnussen, L. Michelsen and A. A. Fredenslund, “Azeotropic Distillation Using UNIFAC,” Chemical Engineering Progress Symposium Series, Vol. 56, No. 4, 1979.</mixed-citation></ref><ref id="scirp.26465-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">M. Rovaglio and F. M. Doherty, “Dynamics of Heterogeneous Azeotropic Distillation Columns,” AIChe Journal, Vol. 36, No. 1, 1990, pp. 39-52.</mixed-citation></ref><ref id="scirp.26465-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">C. J. Wang, D. S. Wong, I.-L. Chien, R. F. Shih, S. J. Wang and C. S. Tsai, “Experimental Investigation of Multiple Steady States and Parametric Sensitivity in Azeotropic Distillation,” Computer and Chemical Engineering, Vol. 21, 1997, pp. S535-S540.</mixed-citation></ref><ref id="scirp.26465-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">W. L. Luyben, “Control of the Heterogeneous Azeotropic n-Butanol/Water,” Energy and Fuels, Vol. 22, No. 6, 2008, pp. 4249-4258. doi:10.1021/ef8004064</mixed-citation></ref><ref id="scirp.26465-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">Y. Wu and I. Chien, “Design and Control of Heterogeneous Azeotropic Column System for the Separation of Pyridine and Water,” Industrial &amp; Engineering Chemistry Research, Vol. 48, No. 23, 2009, pp. 10564-10576.  
doi:10.1021/ie901231s</mixed-citation></ref><ref id="scirp.26465-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">M. Z. Lao and R. Taylor, “Modeling Mass-Transfer in 3-Phase Distillation,” Industrial and Engineering Chemistry Research, Vol. 33, No. 11, 1994, pp. 2637-2650.  
doi:10.1021/ie00035a015</mixed-citation></ref><ref id="scirp.26465-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">S. Widagdo and W. D. Seider, “Azeotropic Distillation,” AIChE Journal, Vol. 42, No. 1, 1996, pp. 96-130.</mixed-citation></ref><ref id="scirp.26465-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">A. Higler, R. Chande, R. Taylor, R. Baur and R. Krishna, “Non-Equilibrium Modeling of Three-Phase Distillation,” Computers and Chemical Engineering, Vol. 28, No. 10, 2004, pp. 2021-2036.  
doi:10.1016/j.compchemeng.2004.04.008</mixed-citation></ref><ref id="scirp.26465-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">B. P. Cairns and I. A. Furzer, “Multicomponent 3-Phase Azeotropic Distillation—Extensive Experimental Data and Simulation Results,” Industrial and Engineering Chemistry Research, Vol. 29, No. 7, 1990, pp. 1349-1363.  
doi:10.1021/ie00103a040</mixed-citation></ref><ref id="scirp.26465-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">T. L. Junqueira, M. O. S. Dias, R. Maciel Filho, M. R. W. Maciel and C. E. V. Rossel, “Simulation of the Azeotropic Distillation for Anhydrous Bioethanol Production: Study on the Formation of a Second Liquid Phase,” Computer Aided Chemical Engineering, Vol. 27, 2009, pp. 1143-1148. doi:10.1016/S1570-7946(09)70411-0</mixed-citation></ref><ref id="scirp.26465-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">A. R. Silva, J. H. P. Brooman, L. R. Braga Jr., L. G. S. Vasconcelos and R. P. Brito, “Steady-State and Dynamics Behavior of an Industrial Azeotropic Distillation Column,” The 6th Italian Conference on Chemical and Process Engineering, Pisa, 8-11 June 2003.</mixed-citation></ref><ref id="scirp.26465-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">B. P. Guedes, M. F. Figueiredo, L. G. S. Vasconcelos, A. C. B. Araújo and R. P. Brito, “Sensitivity and Dynamic Behavior Analysis of an Industrial Azeotropic Distillation Column,” Separation and Purification Technology, Vol. 56, No. 3, 2007, pp. 270-277.  
doi:10.1016/j.seppur.2007.02.014</mixed-citation></ref><ref id="scirp.26465-ref17"><label>17</label><mixed-citation publication-type="other" xlink:type="simple">“Azeotropic Data-III, Advances in Chemistry Series,” In: R. F. Gould, Ed., Advances in Chemistry Series, Vol. 116, American Chemical Society, Washington DC, 1973, pp. 1-6.</mixed-citation></ref><ref id="scirp.26465-ref18"><label>18</label><mixed-citation publication-type="other" xlink:type="simple">Pennsylvania State University, “Dechema Chemistry Data Series,” Deutsche Gesellschaft für Chemisches Aparatewesen, Frankfurt am Main, 1990.</mixed-citation></ref></ref-list></back></article>